JPH11228112A - Ozone generator - Google Patents
Ozone generatorInfo
- Publication number
- JPH11228112A JPH11228112A JP4112198A JP4112198A JPH11228112A JP H11228112 A JPH11228112 A JP H11228112A JP 4112198 A JP4112198 A JP 4112198A JP 4112198 A JP4112198 A JP 4112198A JP H11228112 A JPH11228112 A JP H11228112A
- Authority
- JP
- Japan
- Prior art keywords
- coating
- discharge electrode
- discharge
- ozone
- dielectric constant
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
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Landscapes
- Oxygen, Ozone, And Oxides In General (AREA)
Abstract
(57)【要約】
【課題】 オゾン生成反応に寄与する電界の集中を緩
和し、放電による温度上昇が小さくして、オゾンの2次
分解や、温度上昇で増加する窒素酸化物の生成を抑え、
オゾンの発生効率を向上させたオゾン発生素子を提供す
る。
【解決手段】 誘電体1を挟んで放電電極2と接地電極
3を設け、前記放電電極2の上に保護被膜4をそなえた
オゾン発生素子において、前記保護被膜4が、放電電極
2に接触する第1被膜41と、この第1被膜に重ねた第
2被膜42をそなえ、第1被膜の誘電率より第2被膜の
誘電率を大きくし、電気力線の屈折角度を大きくしてい
る。保護被膜4の層を、順次誘電率を大きくして増すこ
とができる、
(57) [Summary] [PROBLEMS] To alleviate the concentration of an electric field contributing to the ozone generation reaction, reduce the temperature rise due to discharge, and suppress the secondary decomposition of ozone and the generation of nitrogen oxides that increase with the temperature rise. ,
Provided is an ozone generation element having improved ozone generation efficiency. SOLUTION: In an ozone generating element provided with a discharge electrode 2 and a ground electrode 3 with a dielectric 1 interposed therebetween and a protective film 4 provided on the discharge electrode 2, the protective film 4 comes into contact with the discharge electrode 2. A first coating 41 and a second coating 42 superimposed on the first coating are provided. The dielectric constant of the second coating is larger than the dielectric constant of the first coating, and the angle of refraction of the lines of electric force is increased. The layer of the protective coating 4 can be sequentially increased by increasing the dielectric constant,
Description
【0001】[0001]
【発明の属する技術分野】本発明は、沿面放電によりオ
ゾンを発生させるオゾン発生素子に関する。The present invention relates to an ozone generating element for generating ozone by creeping discharge.
【0002】[0002]
【従来の技術】従来、脱臭、殺菌などのために使用され
ている沿面放電式オゾン発生装置は、たとえば図4に示
すように、矢印方向に原料ガスを通すチャンバ10内
に、セラミック、マイカ、ガラスなどの誘電体1を挟ん
で、たとえば厚さ3mmのステンレス鋼板(SUS31
6)を帯状にした放電電極2と、厚さ3mmのステンレ
ス鋼板を放電電極2より広くした接地電極3とを設け、
放電電極2の上に保護被膜4をそなえたオゾン発生素子
を、絶縁板5を介して取り付け、放電電極2と接地電極
3との間に高周波高電圧を印加して、放電電極2上部の
空間で電気絶縁を破壊させて誘電体の沿面方向に沿って
沿面放電6を発生させ、この放電エネルギーでチャンバ
10内の電界領域を通る原料ガス7の中に含まれる酸素
分子の一部をオゾンに転化させるようにしている。2. Description of the Related Art Conventionally, a creepage discharge type ozone generator conventionally used for deodorization, sterilization, and the like, as shown in FIG. For example, a stainless steel plate having a thickness of 3 mm (SUS31
6) a discharge electrode 2 having a strip shape, and a ground electrode 3 having a stainless steel plate having a thickness of 3 mm wider than the discharge electrode 2 are provided.
An ozone generating element provided with a protective film 4 on the discharge electrode 2 is attached via an insulating plate 5, and a high-frequency high voltage is applied between the discharge electrode 2 and the ground electrode 3 to form a space above the discharge electrode 2. A surface discharge 6 is generated along the surface direction of the dielectric by breaking electric insulation, and a part of oxygen molecules contained in the source gas 7 passing through the electric field region in the chamber 10 is converted into ozone by the discharge energy. It is being converted.
【0004】[0004]
【発明が解決しようとする課題】しかるに、このような
オゾン発生素子では、図5に示すように、放電電極2か
ら発する電気力線は、放電電極2から保護被膜4に角度
をθ1 で入り、原料ガス7の空間に抜けるので、電界が
放電電極2の近傍における原料ガス7の一部に集中して
沿面放電6を発生する。このため、この集中した空間部
分の温度が放電によって急激に上昇し、放電によって生
成されたオゾンが熱によって分解されるだけでなく、原
料ガスとして空気を用いる場合は、温度上昇によりオゾ
ンの分解を促進させる窒素酸化物の生成が増大し、オゾ
ン発生装置としての効率を低下させる欠点がある。ま
た、オゾン発生反応に寄与する電界領域が放電電極近傍
の空間に限定されるため、放電の範囲も狭い範囲に限ら
れ、原料ガスとの接触範囲が小さくなり沿面放電式オゾ
ン発生素子のオゾン発生効率が低くなっている。本発明
は、オゾン生成反応に寄与する電界の集中を緩和し、放
電領域を広げることにより、効率よくオゾンを発生させ
るオゾン発生素子を提供することを目的とする。However, in such an ozone generating element, as shown in FIG. 5, electric lines of force generated from the discharge electrode 2 enter the protective film 4 from the discharge electrode 2 at an angle of θ 1 . The electric field concentrates on a part of the source gas 7 in the vicinity of the discharge electrode 2 to generate the creeping discharge 6. For this reason, the temperature of this concentrated space portion rapidly rises due to the discharge, and not only is the ozone generated by the discharge decomposed by heat, but also when air is used as a raw material gas, the ozone is decomposed due to the temperature rise. There is a disadvantage in that the generation of promoted nitrogen oxides increases and the efficiency of the ozone generator decreases. Further, since the electric field region contributing to the ozone generation reaction is limited to the space in the vicinity of the discharge electrode, the discharge range is also limited to a narrow range, the contact range with the raw material gas is reduced, and the ozone generation of the creeping discharge type ozone generation element is reduced. Efficiency is low. An object of the present invention is to provide an ozone generation element that efficiently generates ozone by relaxing concentration of an electric field that contributes to an ozone generation reaction and expanding a discharge region.
【0005】[0005]
【課題を解決するための手段】このため本発明は、放電
電極と接地電極との間に誘電体を有する沿面放電式オゾ
ン発生素子において、前記放電電極の上に設けた保護被
膜を誘電率の異なる2層以上の被膜で形成させ、各層被
膜の誘電率を、放電電極にもっとも近い第1被膜から、
原料ガスにもっとも近い外側の層に向かって順次大きく
なるようにしている。Accordingly, the present invention provides a surface discharge type ozone generator having a dielectric between a discharge electrode and a ground electrode, wherein a protective film provided on the discharge electrode has a dielectric constant. It is formed of two or more different coatings, and the dielectric constant of each coating is determined from the first coating closest to the discharge electrode.
The size is gradually increased toward the outer layer closest to the source gas.
【0006】[0006]
【発明の実施の形態】セラミック、マイカ、ガラスなど
からなる誘電体の一方の面に、高周波高電圧を印加する
放電電極をそなえ、他方の面に接地される接地電極をそ
なえ、前記放電電極の上にセラミックコーティングによ
って均一な厚さに形成した第1被膜を設け、この第1被
膜の上に、誘電率が第1被膜より大きい第2被膜を均一
な厚さで重ねて設けている。また、第1被膜の上に、次
第に誘電率を大きくした複数層の被膜を重ねて設けるこ
とができる。なお、各層の被膜の厚さは、5〜15μm
とし、被膜全体の厚さは10〜30μmにすることが望
ましい。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS One surface of a dielectric made of ceramic, mica, glass, or the like is provided with a discharge electrode for applying a high-frequency high voltage, and the other surface is provided with a ground electrode grounded. A first coating formed by a ceramic coating to have a uniform thickness is provided thereon, and a second coating having a dielectric constant larger than the first coating is provided on the first coating in a uniform thickness. Further, a plurality of layers of films having gradually increased dielectric constants may be provided on the first film. In addition, the thickness of the coating of each layer is 5 to 15 μm.
It is desirable that the thickness of the entire coating be 10 to 30 μm.
【0007】[0007]
【実施例】以下、本発明を図に示す第1の実施例につい
て説明する。なお、図では説明のため被膜の厚さを誇大
にしめしている。図1において、1は電気絶縁性、耐熱
性、熱伝導性のよい材料たとえばアルミナセラミックか
らなる誘電体で、その一方の面に放電電極2と他方の面
に前記放電電極より広くした接地電極3を導電性ペース
トを用いて印刷技術により設けている。4は放電電極2
の保護被膜で、第1被膜41と第2被膜42をそなえて
いる。第1被膜41は放電電極2の上に、比誘電率が1
0程度のアルミナを主成分としたセラミックコーティン
グ劑をスピンコート、スプレー、ディップ、ロールコー
トなどにより8μmの均一な厚さで塗布している。第2
被膜42は、第1被膜の上に設けて第1被膜41よりも
高い誘電率をそなえており、放電による耐食性を考慮し
て比誘電率が100以上の酸化チタンを主成分とするセ
ラミックコーティング劑を用いて10μmの厚さで均一
に塗布形成している。なお、各被膜41、42の厚さ
は、同じ厚さであっても異なる厚さにしてもよいが、5
〜15μmで均一に形成すればよく、第2被膜は高温焼
成することにより各部に熱歪みを生じるおそれがあるの
で、常温硬化の無機コーティング劑を使用し、あるいは
第1被膜を仮焼成し、第2被膜とともに高温焼成するこ
とが好ましい。BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a block diagram showing a first embodiment of the present invention; In the drawings, the thickness of the coating is exaggerated for the sake of explanation. In FIG. 1, reference numeral 1 denotes a dielectric made of a material having good electrical insulation, heat resistance, and heat conductivity, for example, alumina ceramic, and has a discharge electrode 2 on one surface and a ground electrode 3 wider than the discharge electrode on the other surface. Is provided by a printing technique using a conductive paste. 4 is a discharge electrode 2
And a first coating 41 and a second coating 42. The first coating 41 has a relative dielectric constant of 1 on the discharge electrode 2.
A ceramic coating agent containing about 0 as a main component of alumina is applied to a uniform thickness of 8 μm by spin coating, spraying, dipping, roll coating or the like. Second
The coating 42 is provided on the first coating and has a higher dielectric constant than the first coating 41. In consideration of corrosion resistance due to electric discharge, a ceramic coating agent having a relative dielectric constant of 100 or more as a main component is titanium oxide. To form a uniform coating with a thickness of 10 μm. Note that the thickness of each of the coatings 41 and 42 may be the same or different.
The second coating may be formed uniformly at a thickness of about 15 μm, and the second coating may be subjected to high-temperature baking, which may cause thermal distortion in each part. Therefore, use an inorganic coating agent that is cured at room temperature, or temporarily bake the first coating. It is preferable to perform high-temperature baking together with the two coatings.
【0008】この放電電極2と接地電極3との間に図示
しない電源から高周波高電圧を印加すると、第2被膜上
面の原料ガス内で沿面放電を開始し、オゾンを発生す
る。このとき、放電電極2から発する電気力線は、放電
電極2から誘電率E1 の第1被膜に入る角度をθ1 とす
れば、異なる誘電率E2 の第2被膜の界面に入り込むと
きの屈折角θ2 は、 tanθ1/tanθ2=E1/E2 の関係であることから、E1 <E2 であればθ1 <θ2
となり、図2に示すように、電気力線の屈折率は、誘電
率の大きい第2被膜に入ることによって増大し、第2被
膜のない従来の電気力線を示す図5と比較しても明らか
なように、放電による電界が原料ガス7で広がって集中
が緩和される。このため、局部的な放電の発生をなくし
て空間温度の上昇を小さくし、熱によるオゾンの2次分
解や、温度上昇で増加する窒素酸化物の生成を抑えるこ
とができる。また、原料ガス内における放電空間の広が
りにより、原料ガスと電界とが接触する確率が高く、オ
ゾン発生効率が向上する。When a high-frequency high voltage is applied between the discharge electrode 2 and the ground electrode 3 from a power supply (not shown), creeping discharge is started in the raw material gas on the upper surface of the second coating, and ozone is generated. At this time, if the angle of electric lines of force generated from the discharge electrode 2 enters the first film having the dielectric constant E 1 from the discharge electrode 2 as θ 1 , the electric force lines when entering the interface of the second film having the different dielectric constant E 2 refraction angle theta 2 is, tanθ 1 / tanθ 2 = E 1 / E because it is the second relationship, E 1 <E if 2 theta 1 <theta 2
As shown in FIG. 2, the refractive index of the electric flux lines increases by entering the second coating having a large dielectric constant, and is compared with FIG. 5 showing the conventional electric flux lines without the second coating. As is apparent, the electric field due to the discharge spreads in the source gas 7 and the concentration is reduced. For this reason, it is possible to eliminate the occurrence of local discharge and reduce the rise in the space temperature, thereby suppressing the secondary decomposition of ozone due to heat and the generation of nitrogen oxides that increase with the rise in temperature. Further, the probability of contact between the source gas and the electric field is increased due to the expansion of the discharge space in the source gas, and the ozone generation efficiency is improved.
【0009】図3は、第2の実施例で、図1と同じ部分
に同一の符号を付しており、第1被膜41は無機接着剤
を塗布してプリプレグ状態にし、その上に誘電率の高い
セラミックシートを重ねて第2被膜42とし、さらにこ
の第2被膜の上に第2被膜より誘電率が高い無機コーテ
ィング劑で第3被膜43を形成して加熱硬化させてお
り、各層被膜の厚さは5〜15μmとし、保護被膜4全
体の厚さは誘電体1より小さく、30μm程度にしてあ
る。この実施例では、電気力線の屈折を第1の実施例よ
りさらに大きくすることができ、原料ガス内での電界領
域を広くして局部集中を抑えられる。なお、さらに被膜
の層を増すことができるが、製作に手数を考慮し、電界
強度を維持するために、3層あるいは4層程度にするの
がよい。FIG. 3 shows a second embodiment, in which the same parts as those in FIG. 1 are denoted by the same reference numerals, and the first coating 41 is coated with an inorganic adhesive to form a prepreg state. The second coating 42 is formed by stacking high-ceramic sheets, and a third coating 43 is formed on the second coating with an inorganic coating agent having a dielectric constant higher than that of the second coating, and is cured by heating. The thickness is 5 to 15 μm, and the entire thickness of the protective coating 4 is smaller than that of the dielectric 1 and is about 30 μm. In this embodiment, the refraction of the lines of electric force can be further increased as compared with the first embodiment, and the electric field region in the source gas is widened to suppress local concentration. Although the number of coating layers can be further increased, the number of layers is preferably about three or four in order to maintain the electric field strength in consideration of the number of steps in the production.
【0011】[0011]
【発明の効果】このように本発明は、誘電体を挟んで放
電電極と接地電極を設け、前記放電電極の上に保護被膜
をそなえたオゾン発生素子において、前記保護被膜を、
誘電率の異なる複数層の被膜で形成させ、各層被膜の誘
電率を、放電電極に近い被膜から順次大きくしているの
で、電気力線が誘電率の異なる被膜に入るときの屈折角
度が大きくなり、原料ガス層における電界領域が広がっ
て集中を緩和し、放電による温度上昇が小さく、オゾン
の2次分解や、温度上昇で増加する窒素酸化物の生成を
抑えるとともに、原料ガスと電界との接触を良好にし、
オゾンの発生効率を向上させる効果が得られる。As described above, the present invention provides an ozone generating element having a discharge electrode and a ground electrode with a dielectric interposed therebetween, and a protective film provided on the discharge electrode.
The film is formed of multiple layers with different dielectric constants, and the dielectric constant of each layer coating is gradually increased from the one near the discharge electrode, so the angle of refraction when the lines of electric force enter the films with different dielectric constants increases. In addition, the electric field region in the source gas layer is widened and the concentration is relaxed, the temperature rise due to discharge is small, the secondary decomposition of ozone and the generation of nitrogen oxide which increases with the temperature rise are suppressed, and the contact between the source gas and the electric field is suppressed. Good
The effect of improving the ozone generation efficiency is obtained.
【図1】本発明の第1の実施例を示す側断面図である。FIG. 1 is a side sectional view showing a first embodiment of the present invention.
【図2】図1に示す実施例の電気力線を示す特性図であ
る。FIG. 2 is a characteristic diagram showing electric lines of force of the embodiment shown in FIG.
【図3】第2の実施例を示す側断面図である。FIG. 3 is a side sectional view showing a second embodiment.
【図4】オゾン発生装置に取り付けられた状態の従来例
を示す側断面図である。FIG. 4 is a side sectional view showing a conventional example attached to an ozone generator.
【図5】従来の例における電気力線の特性図である。FIG. 5 is a characteristic diagram of electric lines of force in a conventional example.
1 誘電体 2 放電電極 3 接地電極 4 保護被膜 41 第1被膜 42 第2被膜 43 第3被膜 5 絶縁板 6 沿面放電 7 原料ガス 10 チャンバ DESCRIPTION OF SYMBOLS 1 Dielectric 2 Discharge electrode 3 Ground electrode 4 Protective film 41 First film 42 Second film 43 Third film 5 Insulating plate 6 Surface discharge 7 Source gas 10 Chamber
Claims (2)
け、前記放電電極の上に保護被膜をそなえ、電極間に高
周波高電圧を印加して沿面放電を発生させるオゾン発生
素子において、前記保護被膜が、誘電率の異なる2層以
上の被膜で形成され、各層被膜の誘電率を、放電電極に
接触する被膜から、原料ガス層に接触する被膜に向かっ
て順次大きくしたことを特徴とするオゾン発生素子。A discharge electrode and a ground electrode sandwiching a dielectric, a protective coating on the discharge electrode, and applying a high-frequency high voltage between the electrodes to generate a creeping discharge; The protective coating is formed of two or more coatings having different dielectric constants, and the dielectric constant of each coating is sequentially increased from the coating in contact with the discharge electrode toward the coating in contact with the source gas layer. Ozone generator.
mで、全体の厚さが10〜30μmである請求項1また
は2のオゾン発生素子。2. The thickness of each layer of the protective coating is 5 to 10 μm.
The ozone generating element according to claim 1 or 2, wherein m is an overall thickness of 10 to 30 µm.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4112198A JPH11228112A (en) | 1998-02-06 | 1998-02-06 | Ozone generator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4112198A JPH11228112A (en) | 1998-02-06 | 1998-02-06 | Ozone generator |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH11228112A true JPH11228112A (en) | 1999-08-24 |
Family
ID=12599629
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4112198A Pending JPH11228112A (en) | 1998-02-06 | 1998-02-06 | Ozone generator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH11228112A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100712839B1 (en) | 2004-09-14 | 2007-05-02 | 엘지전자 주식회사 | Creeping discharge type air purifier |
| JP2008270110A (en) * | 2007-04-24 | 2008-11-06 | National Institute Of Advanced Industrial & Technology | Surface plasma actuator for high temperature field |
-
1998
- 1998-02-06 JP JP4112198A patent/JPH11228112A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100712839B1 (en) | 2004-09-14 | 2007-05-02 | 엘지전자 주식회사 | Creeping discharge type air purifier |
| JP2008270110A (en) * | 2007-04-24 | 2008-11-06 | National Institute Of Advanced Industrial & Technology | Surface plasma actuator for high temperature field |
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